Electrodynamics of Continuous MediaCovers the theory of electromagnetic fields in matter, and the theory of the macroscopic electric and magnetic properties of matter. There is a considerable amount of new material particularly on the theory of the magnetic properties of matter and the theory of optical phenomena with new chapters on spatial dispersion and non-linear optics. The chapters on ferromagnetism and antiferromagnetism and on magnetohydrodynamics have been substantially enlarged and eight other chapters have additional sections. |
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Page xii
... polarization P Magnetization M Total electric moment of a body 4° Total magnetic moment of a body .4/ Permittivity e Dielectric susceptibility k Magnetic permeability u Magnetic susceptibility X Current density j Conductivity a Absolute ...
... polarization P Magnetization M Total electric moment of a body 4° Total magnetic moment of a body .4/ Permittivity e Dielectric susceptibility k Magnetic permeability u Magnetic susceptibility X Current density j Conductivity a Absolute ...
Page 7
... polarization. Thus C7'11 = 1/C1, CT'12 = 1/r, and similarly CT'22 = 1/C2. Hence we findt C, C C, C C, C co-c (i. #) C12 = - 1-2, co-c (i. 1 1) r r r? f The subsequent terms in the expansion are in general of order (in 1/r) one higher ...
... polarization. Thus C7'11 = 1/C1, CT'12 = 1/r, and similarly CT'22 = 1/C2. Hence we findt C, C C, C C, C co-c (i. #) C12 = - 1-2, co-c (i. 1 1) r r r? f The subsequent terms in the expansion are in general of order (in 1/r) one higher ...
Page 34
... polarization, or simply the polarization, of the body. A dielectric in which P differs from zero is said to be polarized. The vector P determines not only the volume charge density (6.3), but also the density o of the charges on the ...
... polarization, or simply the polarization, of the body. A dielectric in which P differs from zero is said to be polarized. The vector P determines not only the volume charge density (6.3), but also the density o of the charges on the ...
Page 35
... polarization vector is the dipole moment (or electric moment) per unit volume of the dielectric.t Substituting (6.3) in (6.2), we obtain the second equation of the electrostatic field in the form - div D = 0, (6.6) where we have ...
... polarization vector is the dipole moment (or electric moment) per unit volume of the dielectric.t Substituting (6.3) in (6.2), we obtain the second equation of the electrostatic field in the form - div D = 0, (6.6) where we have ...
Page 36
... polarization also is proportional to the field: P = kE = (8–1)E/4t. (7.2) The quantity k is called the polarization coefficient of the substance, or its dielectric susceptibility. Later ($14) we shall show that the permittivity always ...
... polarization also is proportional to the field: P = kE = (8–1)E/4t. (7.2) The quantity k is called the polarization coefficient of the substance, or its dielectric susceptibility. Later ($14) we shall show that the permittivity always ...
Contents
1 | |
34 | |
CHAPTER III STEADY CURRENT | 86 |
CHAPTER IV STATIC MAGNETIC FIELD | 105 |
CHAPTER V FERROMAGNETISM AND ANTIFERROMAGNETISM | 130 |
CHAPTER VI SUPERCONDUCTIVITY | 180 |
CHAPTER VII QUASISTATIC ELECTROMAGNETIC FIELD | 199 |
CHAPTER VIII MAGNETOHYDRODYNAMICS | 225 |
CHAPTER XI ELECTROMAGNETIC WAVES IN ANISOTROPIC MEDIA | 331 |
CHAPTER XII SPATIAL DISPERSION | 358 |
CHAPTER XIII NONLINEAR OPTICS | 372 |
CHAPTER XIV THE PASSAGE OF FAST PARTICLES THROUGH MATTER | 394 |
CHAPTER XV SCATTERING OF ELECTROMAGNETIC WAVES | 413 |
CHAPTER XVI DIFFRACTION OF XRAYS IN CRYSTALS | 439 |
CURVILINEAR COORDINATES | 452 |
INDEX | 455 |
CHAPTER IX THE ELECTROMAGNETIC WAVE EQUATIONS | 257 |
CHAPTER X THE PROPAGATION OF ELECTROMAGNETIC WAVES | 290 |
Other editions - View all
Electrodynamics of Continuous Media: Volume 8 L D Landau,E.M. Lifshitz,L. P. Pitaevskii Snippet view - 1995 |
Common terms and phrases
According angle anisotropy assumed averaging axes axis becomes body boundary conditions calculation called charge coefficient compared components condition conducting conductor consider constant continuous coordinates corresponding crystal curl denote density depends derivative determined dielectric direction discontinuity distance distribution effect electric field ellipsoid energy equal equation expression external factor ferromagnet fluid flux follows force formula frequency function given gives grad Hence incident increases independent induction integral linear magnetic field mean medium neglected normal obtain occur parallel particle particular permittivity perpendicular phase plane polarization positive potential present PROBLEM propagated properties quantities range regarded region relation respect result rotation satisfied scattering simply solution sphere Substituting surface symmetry taken temperature tensor theory thermodynamic transition uniform unit values variable vector volume wave write zero